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26 Jul 2013: Although suchcooperative effects have already been demonstrated forcoupled active but non-self-propelled particles in severaldifferent contexts 24–26, the generalization of our resultsto a large number of active particles remains ... Weinheim, Ger. 19,

26 Jul 2013: 061701-2 Michelin, Lauga, and Bartolo Phys. Fluids 25, 061701 (2013). by interfacial stresses arising from the self-generated gradients of reactive surfactants.21, 24, 25 Unlikeautophoretic Janus particles, which swim ... Mater. 24, 811–816 (2012).7 P.

26 Jul 2013: also include an induced electrophoreticcomponent,24 proportional to their zeta potential and thestreaming electric field. ... Up(z) ) Uhydro(z) Uelec(z) UkBT (24). Uhydro(z) ) [1 - O(ad)]UPD(z)ex (25).

26 Jul 2013: metrical model for dinoflagellates.24,25 A dinoflagellate can. FIG. 1. (Color online) (a) Notation for. ... Julicher, “Generic aspects of axonemal beating,” New J. Phys. 2, 24 (2000).11T.

26 Jul 2013: However, as expected, thecapillary attraction leads to an additional compressive load (theUk2 term in eqn (24)). ... 1999, 82, 1991.24 B. J. Reynwar, G. Illya, V. A. Harmandaris, M.

26 Jul 2013: without tail flexibilityno swimming can occur.5, 24 The second swimmer has a flat rubber tail (L = 20.5 mm, thickness t= 0.8 mm, width w = 3.4 mm, E = ... Rev. Lett. 80, 3879–3882 (1998).24 See supplementary material at

26 Jul 2013: Here, the first effect of inertia is the appear-ance of a lift force directed across the undisturbedstreamlines.13,23,24 The original study, due to Saffman,23,24.

26 Jul 2013: Fluid Mech. 24, 313–358 (1992). 071904-16 Y. Man and E. Lauga Phys. ... Soft Matter 7, 8169–8181 (2011).24 L. Zhang, K. E. Peyer, and B.

26 Jul 2013: be. L. L. a. V(z). Wetted. 0 s. 0 s. 24.5 s. ... Phys. Rev. Lett. 96, 186102 (2006).23. Squires, T. M. Phys. Fluids 20, 092105 (2008).24.

26 Jul 2013: J2k1/2(2πMa) cos 2kψ cos 2nψ (k 0). (2.24). Equation (2.24) is a symmetric infinite system of linear equations for the coefficients{cn; n 0}. ... The correspondingsolution of (2.24) is. c0 =4a. 3π. DL, cn = 0 (n > 0), (2.29).

26 Jul 2013: One such model is con-sidered in the discussion FENE-P, and we obtain the sameresults see also 24. ... S. Suarez and X. B. Dai, Biol. Reprod. 46, 686 1992.24 E.

26 Jul 2013: 9500 Gillman Drive, La Jolla California 92093-0411, USA(Received 15 January 2008; published 24 July 2008). ... J. Pedley and J. O. Kessler, Annu. Rev. Fluid Mech. 24,.

26 Jul 2013: 2010).[19] S. Camalet and F. Jülicher, New J. Phys. 2, 24 (2000). ... Phys. 46, 13 (1997).[24] T. R. Powers, Rev. Mod. Phys. 82, 1607 (2010).[25] L.

26 Jul 2013: By scaling timesby 9. 5122f 24 / 21 and numbering the particles along the. ... 24 and 25 to ex-plicitly obtain at leading order in 1 / di j.

26 Jul 2013: Typical two-dimensional (a) and three-dimensional (b),(c) cilium kinematics as observed forPleurobrachia [24] and Mytilus edulis [25], respectively.Sketch of the coordinates (d) and of the forces and momentsthat ... Kung, J. Cell Biol. 87, 33 (1980).[24]

26 Jul 2013: Received 20 March 2007; accepted 16 May 2007; published online 24 August 2007. ... 083104-2 Eric Lauga Phys. Fluids 19, 083104 2007. Downloaded 24 Aug 2007 to 128.54.43.238.

26 Jul 2013: Langmuir 24, 12158–12163.BATCHELOR, G. K. 1972 Sedimentation in a dilute dispersion of spheres. ... Annu. Rev. Fluid Mech. 24, 313–358. PHONGIKAROON, S., HOFFMASTER, R., JUDD, K.

11 Nov 2013: un1 = un t. 24(9Fn1 19Fn 5Fn1 Fn2). NB uses 1 function evaluation per step – goodNB difficult to start or change step size t – badNB Stable t.

26 Jul 2013: F =1. 4. y02ISp. Sp4, 24. where ISp is a dimensionless integral defined by. ... 24, the measure-ments would show a decrease in the propulsive force nearboundaries.

12 Nov 2013: 22 4.000000302 3.015609e-07 0.5011010 1.0482393. 23 4.000000147 1.467238e-07 0.4865479 1.0479823. 24 4.000000064 6.370571e-08 0.4341880 1.0530215.